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How do actual vapor power cycles differ from idealized ones?

Short Answer

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Answer: Actual vapor power cycles differ from idealized cycles in terms of the efficiency and performance of their components, such as boilers, turbines, condensers, and pumps. In actual cycles, there are energy losses at different stages, like heat loss, pressure losses, and irreversibilities in processes, which do not occur in idealized cycles. Furthermore, actual vapor power cycles have less than 100% efficiency for components like turbine, pump, and heat exchangers, while in idealized cycles, the efficiencies are assumed to be perfect. Actual cycles may also include additional components such as multiple turbine stages, reheaters, and feedwater heaters to improve performance, which may not be present in idealized cycles.

Step by step solution

01

Overview of Vapor Power Cycles

Vapor power cycles are a series of processes that convert heat into work, commonly used in power plants to generate electricity. These cycles typically involve the working fluid evaporating and condensing within the cycle to recover the latent heat of vaporization. An idealized vapor power cycle represents the ideal process with no energy losses and perfect efficiency, while an actual vapor power cycle accounts for the real-world losses and inefficiencies.
02

Main Components in Both Cycles

Both actual and idealized vapor power cycles consist of the same four main components: a boiler or steam generator, a turbine, a condenser, and a pump. However, the efficiency and performance of these components in actual cycles are lower than in the idealized ones.
03

Energy Losses in Real Components

In actual vapor power cycles, there are energy losses at different stages, which do not occur in idealized cycles. Some of these energy losses include: 1. Heat loss through the walls of the boiler, turbine, condenser, and pump. 2. Pressure losses across the pipes and components due to friction. 3. Irreversibilities in heat transfer and work extraction processes.
04

Difference in Efficiencies

In an idealized vapor power cycle, it is assumed that the components are perfectly efficient, i.e., the turbine and pump isentropic efficiencies are 100%, and heat transfer processes occur without any losses. In an actual vapor power cycle, these assumptions do not hold, and the efficiencies of the turbine, pump, and heat exchangers are less than 100%, leading to a decrease in cycle efficiency.
05

Other Design Differences

In actual vapor power cycles, additional components may be introduced to improve performance, which may not be present in an idealized cycle. For example, real power plants often use multiple stages of turbines, reheaters, and feedwater heaters to gain maximum efficiency, whereas an idealized cycle may represent only a simple Rankine cycle without these enhancements. In conclusion, actual vapor power cycles differ from idealized ones due to the real-world inefficiencies, energy losses, and design variations that seek to optimize performance. Although an idealized cycle provides a useful theoretical reference, understanding the actual cycle is necessary to effectively design and operate real-world power plants.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Ideal vs Real Vapor Power Cycles
When considering the efficiency of power generation, it's critical to differentiate between ideal and real vapor power cycles. An ideal vapor power cycle operates under hypothetical conditions where there are no energy losses—meaning that all the energy from the heat source is converted into mechanical work. Imagine the perfection of a frictionless world: no heat escapes, every process is reversible, and every component operates at maximum capacity.

In contrast, real vapor power cycles encompass unavoidable inefficiencies due to factors such as friction, heat loss, and material limitations. During the actual operation of a power plant, the boiler, turbine, condenser, and pump all face energy losses. This could include, for example, heat loss through component walls or pressure drops due to friction in the pipes. Thus, while an ideal cycle is a valuable benchmark for theoretical performance, real cycles reflect the practical limitations we must address in engineering.
Cycle Efficiency
The term cycle efficiency is a measure of how effectively a vapor power cycle converts heat into work. In a perfect world, a cycle's efficiency would be 100%, but that's not feasible due to the second law of thermodynamics which indicates all processes incur some inefficiency.

In actual cycles, factors like isentropic efficiency of turbines and pumps come into play—these are never 100% in real-world setups. The real isentropic efficiency reflects how closely a device approaches an ideal, reversible process. The higher the isentropic efficiency, the closer the device is to the ideal, and the higher the overall cycle efficiency. Improvements in the design, such as employing multiple stages of turbines, can increase efficiency, but it's important to remember that no real power cycle can ever reach the perfection of its ideal counterpart.
Energy Losses in Power Cycles
Understanding and mitigating energy losses in power cycles is key to improving efficiency. In the real world, energy losses occur at every step of the vapor power cycle. These energy losses stem from a variety of sources: thermal losses through the walls of equipment, pressure drops due to fluid friction in pipes, and irreversible processes during heat transfer and work extraction.

To reduce these losses, engineers implement advanced materials with better insulation properties, design systems to minimize friction and pressure drops, and use techniques like regenerative feedwater heating to recover some of the energy that would otherwise be dissipated as waste heat. Keeping such losses to a minimum is not only an engineering challenge but also an economic one, as minimizing these losses leads to lower operating costs and improved environmental outcomes.
Rankine Cycle
The Rankine cycle is a fundamental concept within vapor power cycles and is widely used as the ideal model for steam power plants. It consists of four main stages: the pumping of the working fluid (water) to high pressure, the boiling of water to form steam in the boiler, the expansion of the steam through a turbine to generate power, and the condensation of the steam back into water.

While an ideal Rankine cycle suggests maximum efficiency without any losses, real Rankine cycles introduce several modifications to approach the ideal. These include the addition of reheaters and feedwater heaters, which increase the average temperature at which heat is added, and implementing multiple turbine stages to incrementally convert steam's energy into work. By understanding both the ideal cycle and the real systems' intricacies, students can appreciate the complexities of real-world power generation and the pursuit of increased efficiency.

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Most popular questions from this chapter

The closed feed water heater of a regenerative Rankine cycle is to heat 7000 kPa feed water from \(260^{\circ} \mathrm{C}\) to a saturated liquid. The turbine supplies bleed steam at \(6000 \mathrm{kPa}\) and \(325^{\circ} \mathrm{C}\) to this unit. This steam is condensed to a saturated liquid before entering the pump. Calculate the amount of bleed steam required to heat \(1 \mathrm{kg}\) of feed water in this unit.

A steam power plant operates on an ideal reheat Rankine cycle between the pressure limits of \(15 \mathrm{MPa}\) and 10 kPa. The mass flow rate of steam through the cycle is \(12 \mathrm{kg} / \mathrm{s} .\) Steam enters both stages of the turbine at \(500^{\circ} \mathrm{C}\) If the moisture content of the steam at the exit of the low pressure turbine is not to exceed 10 percent, determine \((a)\) the pressure at which reheating takes place, ( \(b\) ) the total rate of heat input in the boiler, and \((c)\) the thermal efficiency of the cycle. Also, show the cycle on a \(T\) -s diagram with respect to saturation lines.

Steam enters the high-pressure turbine of a steam power plant that operates on the ideal reheat Rankine cycle at 800 psia and \(900^{\circ} \mathrm{F}\) and leaves as saturated vapor. Steam is then reheated to \(800^{\circ} \mathrm{F}\) before it expands to a pressure of 1 psia. Heat is transferred to the steam in the boiler at a rate of \(6 \times 10^{4}\) Btu/s. Steam is cooled in the condenser by the cooling water from a nearby river, which enters the condenser at \(45^{\circ} \mathrm{F}\). Show the cycle on a \(T\) -s diagram with respect to saturation lines, and determine ( \(a\) ) the pressure at which reheating takes place, \((b)\) the net power output and thermal efficiency, and \((c)\) the minimum mass flow rate of the cooling water required.

A steam power plant operates on an ideal reheat regenerative Rankine cycle with one reheater and two feedwater heaters, one open and one closed. Steam enters the high-pressure turbine at \(15 \mathrm{MPa}\) and \(600^{\circ} \mathrm{C}\) and the low-pressure turbine at 1 MPa and \(500^{\circ} \mathrm{C}\). The condenser pressure is 5 kPa. Steam is extracted from the turbine at \(0.6 \mathrm{MPa}\) for the closed feedwater heater and at 0.2 MPa for the open feedwater heater. In the closed feedwater heater, the feedwater is heated to the condensation temperature of the extracted steam. The extracted steam leaves the closed feedwater heater as a saturated liquid, which is subsequently throttled to the open feedwater heater. Show the cycle on a \(T-s\) diagram with respect to saturation lines. Determine \((a)\) the fraction of steam extracted from the turbine for the open feedwater heater, \((b)\) the thermal efficiency of the cycle, and \((c)\) the net power output for a mass flow rate of \(42 \mathrm{kg} / \mathrm{s}\) through the boiler

Refrigerant-134a is used as the working fluid in a simple ideal Rankine cycle which operates the boiler at \(2000 \mathrm{kPa}\) and the condenser at \(24^{\circ} \mathrm{C}\). The mixture at the exit of the turbine has a quality of 93 percent. Determine the turbine inlet temperature, the cycle thermal efficiency, and the back-work ratio of this cycle.

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